The Schwebsite

About “me”

All Thingz Schwemz

“So far as the theories of mathematics are about reality, they are not certain; so far as they are certain, they are not about reality.”

-Albert Einstein

Publications

  1. Piszczatowski RT*, Schwenger E*, Sundaravel S, Stein CM, Liu Y, Stanley P, Verma A, Zheng D, Seidel RD, Almo SC, Townley RA, Bülow HE, Steidl U. A glycan-based approach to cell characterization and isolation: Hematopoiesis as a paradigm. J Exp Med. 2022 Nov 7;219(11):e20212552. doi: 10.1084/jem.20212552. Epub 2022 Sep 6. *Authors contributed equally to this work

  2. Schwenger E, Steidl U. An evolutionary approach to clonally complex hematologic disorders. Blood Cancer Discov. 2021 May;2(3):201-215. doi: 10.1158/2643-3230.BCD-20-0219. Epub 2021 Apr 15.

  3. Ueda K, Kumari R, Schwenger E, Wheat JC, Bohorquez O, Narayanagari SR, Taylor SJ, Carvajal LA, Pradhan K, Bartholdy B, Todorova TI, Goto H, Sun D, Chen J, Shan J, Song Y, Montagna C, Xiong S, Lozano G, Pellagatti A, Boultwood J, Verma A, Steidl U. MDMX acts as a pervasive preleukemic-to-acute myeloid leukemia transition mechanism. Cancer Cell. 2021 Apr 12;39(4):529-547.e7. doi: 10.1016/j.ccell.2021.02.006. Epub 2021 Mar 4.

  4. Schwenger E, Reddy VP, Moorthy G, Sharma P, Tomkinson H, Masson E, Vishwanathan K. Harnessing Meta-analysis to Refine an Oncology Patient Population for Physiology-Based Pharmacokinetic Modeling of Drugs. Clin Pharmacol Ther. 2018 Feb;103(2):271-280. doi: 10.1002/cpt.917. Epub 2017 Nov 20.

  5. Mbogning J, Pagé V, Burston J, Schwenger E, Fisher RP, Schwer B, Shuman S, Tanny JC. Functional interaction of Rpb1 and Spt5 C-terminal domains in co-transcriptional histone modification. Nucleic Acids Res. 2015 Nov 16;43(20):9766-75. doi: 10.1093/nar/gkv837. Epub 2015 Aug 14.

Professional Experience

Lab Experience

Paintings

Notes

“Calculus required continuity, and continuity required the idea of the infinitely little, but nobody could discover what the infinitely little might be.”

-Bertrand Russell

Formulas

Euler’s formula

\(e^{i\pi}=-1\)

Taylor series raised to power of a matrix \(\mathbf{A}\)

\(e^{\mathbf{A}}=\mathbf{A}^0 + \mathbf{A}^1 + \dfrac{1}{2}\mathbf{A}^2 + \dfrac{1}{6}\mathbf{A}^3 + \dfrac{1}{24}\mathbf{A}^4 + ... + \dfrac{1}{n!}\mathbf{A}^n=\) stable matrix.

Schrödinger Equation, \(i\hslash\dfrac{\delta}{\delta t}|\psi\rangle=H|\psi\rangle\)

THe Schrödinger equation in all its glory:

\[\begin{aligned} i\hslash\dfrac{\delta}{\delta t}|\psi\rangle=H|\psi\rangle \end{aligned}\]

, where \(|\psi\rangle\) is the state of the system as a vector (of important parameters such as position and momentum).

Plots

Taylor Expansion, \(cos(x)\)

Fourier Transform, \(\dfrac{cosn\pi x}{n}\)

Essence of calculus

Essence of Calculus

Differential Equations

Differential Equations

Taylor Expansions

Taylor Expansions

Non-Linear Dynamics and Chaos

ChaoOooOOooOoOoooS

Lorenz Attractors

Lorenz Attractors